JPH05280882A - Heat dissipating fin - Google Patents

Heat dissipating fin

Info

Publication number
JPH05280882A
JPH05280882A JP10576592A JP10576592A JPH05280882A JP H05280882 A JPH05280882 A JP H05280882A JP 10576592 A JP10576592 A JP 10576592A JP 10576592 A JP10576592 A JP 10576592A JP H05280882 A JPH05280882 A JP H05280882A
Authority
JP
Japan
Prior art keywords
needle
fin group
pin fin
shaped heat
heat transfer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP10576592A
Other languages
Japanese (ja)
Inventor
Hiroshi Mizukami
浩 水上
Sadashige Mochizuki
貞成 望月
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Toshiba Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Toshiba Corp filed Critical Toshiba Corp
Priority to JP10576592A priority Critical patent/JPH05280882A/en
Publication of JPH05280882A publication Critical patent/JPH05280882A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain a heat dissipating fin in which a heat transfer amount of a pin fin group can be obtained in a high efficiency state by reducing waste of pressure loss. CONSTITUTION:An arranging interval (a) of a pin fin group 11, in which needlelike thermal conductors 13 are arranged in a rectangular state, perpendicular to an air flow is set to a range of 1-1.5 times as large as a length of an outer periphery of the conductor 13. A volume occupied by the conductors 13 is set to 20% or less of an envelope volume of the group 11.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、空調器をはじめとする
各種の放熱器や熱交換器、或いは電算機等の集積回路の
チップやその他の発熱体の放熱に利用される放熱フィン
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a radiator fin used for radiating heat from various radiators and heat exchangers including air conditioners, chips of integrated circuits such as computers, and other heating elements.

【0002】[0002]

【従来の技術】近年、計算機の高速化や小型化に伴う集
積回路のチップ等の高度冷却技術などで、高性能放熱フ
ィンの要求が高まって来ており、伝熱面の微細化に適し
た多角形断面の針状熱伝導体(ピンフィン)を多数本平
行に矩形配列することによりピンフィン群を構成してな
る放熱フィンが着目されている。
2. Description of the Related Art In recent years, there has been an increasing demand for high-performance heat radiation fins due to advanced cooling technology for integrated circuit chips, etc., which is accompanied by the speeding up and downsizing of computers, and is suitable for miniaturization of the heat transfer surface. Attention has been focused on a radiation fin that is formed by arranging a large number of needle-shaped heat conductors (pin fins) having a polygonal cross section in parallel with each other in a rectangular shape.

【0003】図3にこの種の放熱フィンのピンフィン群
1を示す。このピンフィン群1は基板部2上に多数本の
針状熱伝導体3を相互に間隔を存して矩形配列する状態
に立設した構成である。これら各針状熱伝導体3は、図
4に拡大して示す如く、断面四角形で一辺dpが0.2mm 程
度の微細角柱形状とされていると共に、伝熱量(放熱
量)を高くするために高密度に配列されている。即ち、
この縦横の配列間隔(ピッチ)pが狭く設定されてい
る。
FIG. 3 shows a pin fin group 1 of this type of heat radiation fin. The pin fin group 1 has a structure in which a large number of needle-shaped heat conductors 3 are erected on a substrate portion 2 in a rectangular array with a space therebetween. As shown in the enlarged view of FIG. 4, each of the needle-shaped heat conductors 3 has a quadrangular cross section and a fine prismatic shape with one side dp of about 0.2 mm, and is high in order to increase the heat transfer amount (heat dissipation amount). They are arranged in a density. That is,
The vertical and horizontal arrangement intervals (pitch) p are set to be narrow.

【0004】[0004]

【発明が解決しようとする課題】ところで、前述の従来
のピンフィンタイプの放熱フィンでは、伝熱量を高くす
るために、多数本の角柱形状の針状熱伝導体3を高密度
に矩形配列してピンフィン群1を構成していた。つま
り、伝熱量を優先して試行錯誤的に縦横の配列間隔(ピ
ッチ)pを決定していた。その結果、配列間隔pが針状
熱伝導体3の横断面の外周長の1/2 以下(角柱の一辺の
長さdpの2倍以下)になっているのが現状で、後述する
実験結果による針状熱伝導体3の配列間隔pと熱伝達・
圧力損失特性との関係から明らかなように、送風器から
送風せしめられる空気の圧力損失が極めて大きく、全体
評価としては効率が悪い問題があった。
By the way, in the above-mentioned conventional fin fin type heat radiation fin, in order to increase the amount of heat transfer, a large number of prismatic needle-shaped heat conductors 3 are arranged in a high density rectangular shape. It constituted the pin fin group 1. That is, the vertical and horizontal arrangement intervals (pitch) p are determined by trial and error by giving priority to the amount of heat transfer. As a result, the array interval p is 1/2 or less of the outer peripheral length of the cross section of the needle-shaped heat conductor 3 (twice or less of the length dp of one side of the prism) under the present circumstances. And the heat transfer between the needle-shaped heat conductors 3
As is clear from the relationship with the pressure loss characteristics, the pressure loss of the air blown from the blower was extremely large, and there was a problem of poor efficiency as a whole evaluation.

【0005】本発明は前記問題を解決するためになされ
たもので、その目的とするところは、ピンフィン群の伝
熱量を高く維持すると共に、無駄な圧力損失を少なくで
きて、非常に効率の良い伝熱効果が得られる放熱フィン
を提供することにある。
The present invention has been made to solve the above problems, and an object thereof is to maintain a high heat transfer amount in the pin fin group and reduce unnecessary pressure loss, which is very efficient. It is to provide a radiation fin that can obtain a heat transfer effect.

【0006】[0006]

【課題を解決するための手段】本発明の放熱フィンは、
前記目的を達成するために、ピンフィン群の矩形配列さ
れた多角形断面の多数本の針状熱伝導体の少なくとも一
方向の配列間隔を、該針状熱伝導体の横断面の外周長の
1〜1.5 倍の範囲内に設定したことを特徴とする。
The heat radiation fin of the present invention comprises:
In order to achieve the above-mentioned object, the arrangement interval of at least one direction of a large number of pin-shaped fin-shaped heat conductors having a polygonal cross-section is defined as 1 perimeter of the cross-section of the needle-shaped heat conductors. It is characterized by being set within the range of up to 1.5 times.

【0007】[0007]

【作用】前記構成の放熱フィンでは、ピンフィン群の多
角形断面の針状熱伝導体の配列間隔が該針状熱伝導体の
横断面の外周長の1〜1.5 倍の範囲とした方向を空気の
流れに対し直角方向に向けて使用すれば、後述するパラ
メータ試験による針状熱伝導体の配列間隔と熱伝達・圧
力損失特性との関係から分かるように、ピンフィン群の
伝熱量を比較的高く維持すると共に、無駄な圧力損失を
大幅に少なくでき、総合的に非常に効率の良い伝熱効果
が得られて、高効率的な放熱器や熱交換器の実現が可能
となる。
In the radiating fin having the above-described structure, the arrangement interval of the needle-shaped heat conductors of the polygonal cross section of the pin fin group is in the range of 1 to 1.5 times the outer peripheral length of the cross section of the needle-shaped heat conductors. If it is used in the direction perpendicular to the flow, the heat transfer amount of the pin fin group is relatively high, as can be seen from the relationship between the arrangement interval of the needle-shaped heat conductors and the heat transfer / pressure loss characteristics by the parameter test described later. While maintaining it, wasteful pressure loss can be greatly reduced, a highly efficient heat transfer effect can be obtained overall, and a highly efficient radiator or heat exchanger can be realized.

【0008】そのピンフィン群の針状熱伝導体の空気の
流れに直角方向の配列間隔が前述の外周長の1倍より小
さい従来品のようなものでは、伝熱性能は大きく得られ
るが、圧力損失がより大きな割合で増大して、全体評価
として効率が悪くなり、逆に外周長の1.5 倍より大きく
なると、圧力損失は小さいが伝熱量が大幅に減少して放
熱性能の悪化を招く。
In a conventional product in which the needle fin heat conductor of the pin fin group has an arrangement interval in the direction perpendicular to the air flow of less than one time the outer peripheral length described above, a large heat transfer performance can be obtained, but the pressure If the loss increases at a larger rate and the overall evaluation becomes less efficient, and conversely becomes greater than 1.5 times the outer circumference length, the pressure loss will be small but the amount of heat transfer will significantly decrease, leading to poor heat dissipation performance.

【0009】また、前述の如くピンフィン群の多角形断
面の針状熱伝導体の空気の流れに対し直角方向の配列間
隔が該針状熱伝導体の横断面の外周長の1〜1.5 倍の範
囲とした構成の放熱フィンにおいて、ピンフィン群の多
数本の針状熱伝導体の占める体積を、該ピンフィン群の
包絡体積の20%以下にすることで、即ち針状熱伝導体空
気の流れ方向の配列間隔を、該針状熱伝導体の横断面の
外周長の0.35 倍程以上とすることで、これ以上大きな
配列間隔の場合のように空気流の異常な攪乱状態の発生
による圧力損失の過剰な増大を招くことが防げて、より
効率の良い最適な配列構造となる。
Further, as described above, the arrangement interval in the direction perpendicular to the air flow of the needle-shaped heat conductor having the polygonal cross section of the pin fin group is 1 to 1.5 times the outer peripheral length of the cross section of the needle-shaped heat conductor. In the radiating fins having the range configuration, the volume occupied by many needle-shaped heat conductors of the pin fin group is set to 20% or less of the envelope volume of the pin fin group, that is, the needle-shaped heat conductor air flow direction. By making the arrangement interval of 0.35 times or more of the outer peripheral length of the cross section of the needle-shaped heat conductor, the pressure loss due to the occurrence of an abnormal disturbance state of the air flow as in the case of a larger arrangement distance than this It is possible to prevent an excessive increase, resulting in a more efficient and optimal array structure.

【0010】[0010]

【実施例】以下、図面を参照して本発明の放熱フィンの
実施例を説明する。まず、図1は本発明の放熱フィンの
ピンフィン群11の一部省略した平面図で、このピンフ
ィン群11は銅の薄板を材料としてエッチング技術を応
用して製作した断面四角形で一辺dpが0.2mm 程度の微細
角柱形状の針状熱伝導体13を多数本相互に間隔を存し
矩形配列してなる。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the heat radiation fin of the present invention will be described below with reference to the drawings. First, FIG. 1 is a plan view in which a part of the pin fin group 11 of the heat dissipation fin of the present invention is partially omitted. The pin fin group 11 is a quadrangular cross section manufactured by applying an etching technique using a thin copper plate as a material and one side dp is 0.2 mm. A large number of fine prismatic needle-shaped heat conductors 13 are arranged in a rectangular shape with an interval therebetween.

【0011】このピンフィン群11の針状熱伝導体13
の配列間隔(空気の流れに対し直角方向の配列間隔a、
空気の流れ方向の配列間隔b)が、後述するパラメータ
試験の熱伝達・圧力損失特性との関係から解明した最適
値(最も効率の良い値)に設定されている。即ち、この
ピンフィン群11の針状熱伝導体13の空気の流れに対
し直角方向の配列間隔aが該針状熱伝導体13の横断面
の外周長の1.25倍、即ち角柱の一辺の長さdpの5倍(a
/dp=5.0 )に、空気の流れ方向の配列間隔bが該針状
熱伝導体13の横断面の外周長の0.5 倍、即ち角柱の一
辺の長さdpの2.0 倍(b/dp=2.0 )に設定され、これ
ら針状熱伝導体13がピンフィン群11の包絡体積に占
める体積割合が20%以下となっている。
The needle-shaped heat conductor 13 of the pin fin group 11
Array spacing (array spacing a in the direction perpendicular to the air flow,
The arrangement interval b) in the air flow direction is set to the optimum value (the most efficient value) clarified from the relationship with the heat transfer / pressure loss characteristics of the parameter test described later. That is, the arrangement interval a in the direction perpendicular to the air flow of the needle-shaped heat conductor 13 of the pin fin group 11 is 1.25 times the outer peripheral length of the cross section of the needle-shaped heat conductor 13, that is, the length of one side of the prism. 5 times dp (a
/Dp=5.0), the arrangement interval b in the air flow direction is 0.5 times the outer circumferential length of the cross section of the needle-shaped heat conductor 13, that is, 2.0 times the length dp of one side of the prism (b / dp = 2.0). ), The volume ratio of these needle-shaped heat conductors 13 to the envelope volume of the pin fin group 11 is 20% or less.

【0012】こうした構成の配列間隔(ピンピッチ)a
/dp=5.0 、b/dp=2.0 が最も効率的であるとの根拠
となる実験例を述べる。この実験に供試したピンフィン
群は、断面四角形で一辺dpが0.2mm 程度の微細角柱形状
の針状熱伝導体13の空気の流れに直交する方向の配列
間隔a/dpを3.0 〜7.0 の範囲で、流れ方向の配列間隔
b/dpを1.5 〜6.0 の範囲で系統的に変化させたもの
で、これらを改良シングルブロウ法に基づく伝熱特性自
動計測システムを用いパラメータ試験を行った。
The arrangement interval (pin pitch) a having such a configuration
Described below is an experimental example that is based on the fact that /dp=5.0 and b / dp = 2.0 are the most efficient. The pin fin group tested in this experiment has a quadrangular cross section and a fine prismatic needle-shaped heat conductor 13 having a side dp of about 0.2 mm and an array spacing a / dp in the direction of orthogonal to the air flow of 3.0 to 7.0. Then, the arrangement interval b / dp in the flow direction was systematically changed in the range of 1.5 to 6.0, and a parameter test was performed using an automatic measurement system for heat transfer characteristics based on the improved single blow method.

【0013】この試験結果から得られた針状熱伝導体の
各種配列間隔a/dp,b/dpと,熱伝達・圧力損失特性
との関係を図2に示している。ここでは、縦軸にピンフ
ィン群の単位包絡体積・単位温度差あたりの伝熱量E
を、横軸に送風機の単位包絡体積あたりの送風動力(ピ
ンフィン群の圧力損失と比例)Pをあらわしている。い
ずれもピンフィン群への空気の近寄り流速U1は、LS
Iなどの放熱器として用いられる場合に一般的である2
m/sとした場合である。そのEとPとの定義は次の通
りである。
FIG. 2 shows the relationship between the various arrangement intervals a / dp, b / dp of the needle-shaped heat conductor obtained from the test results and the heat transfer / pressure loss characteristics. Here, the vertical axis represents the heat transfer amount E per unit envelope volume / unit temperature difference of the pin fin group.
And the horizontal axis represents the blasting power (proportional to the pressure loss of the pin fin group) P per unit envelope volume of the blower. In both cases, the approaching flow velocity U1 of air to the pin fin group is LS
It is common when used as a radiator of I etc. 2
This is the case of m / s. The definitions of E and P are as follows.

【0014】 E=hm・A/V;P=△P・U1・Az/V hm:平均伝熱量(フィン効率を含まず)、A:伝熱面
積、 V:ピンフィン包絡体積、Az:ピンフィン群入口面積
(ダクト断面積) なお、図中△はa/dp=3.0 、□はa/dp=4.0 、▽は
a/dp=5.0 、◇はa/dp=6.0 、○はa/dp=7.0
で、いずれも空気流れに対し直角方向の配列間隔を示し
ている。また図中[]内の数値は空気流れ方向の配列間
隔b/dp値を示しいている。
E = hm · A / V; P = ΔP · U1 · Az / V hm: Average heat transfer amount (not including fin efficiency), A: Heat transfer area, V: Pin fin envelope volume, Az: Pin fin group Inlet area (duct cross-sectional area) In the figure, △ is a / dp = 3.0, □ is a / dp = 4.0, ▽ is a / dp = 5.0, ◇ is a / dp = 6.0, and ○ is a / dp = 7.0.
In each case, the array spacing in the direction perpendicular to the air flow is shown. In addition, the numerical value in [] in the figure shows the array interval b / dp value in the air flow direction.

【0015】ここで、放熱フィンとして高性能なもの
は、伝熱性能が大きく、同時に圧力損失が小さいもので
あるから、本図においてはPが小さく、Eが大きい値を
示すピン配列間隔のものが最も総合的性能に優れている
ピンフィン群であると言える。この観点から見ると、配
列間隔が狭い△印のa/dp=3.0 の場合、伝熱性能は大
きいが、それにもまして圧力損失が非常に大きいことが
分かる。逆に配列間隔が広い○印のa/dp=7.0 の場合
は伝熱面の稠密度が小さくなり、単位体積あたりの放熱
量がかなり小さくなる。よって、このデータの中間の▽
印のa/dp=5.0のものが総合的性能で最も良い配列ピ
ッチ構造であると言える。▽印のa/dp=5.0 及び◇印
のa/dp=6.0 の場合、空気流れ方向の配列間隔b/dp
の変化が総合性能に及ぼす影響は小さいが、b/dpを2
〜4.5 程度としたものの場合が若干であるが総合性能が
高くなっているのが分かる。これは△印のa/dp=3.0
や□印のa/dp=4.0 の場合にも該当する。
Here, since a high-performance radiating fin has a high heat transfer performance and a small pressure loss at the same time, in this figure, P has a small value and E has a large pin arrangement interval. Can be said to be the pin fin group with the best overall performance. From this point of view, when Δ / a = dp = 3.0, where the arrangement interval is narrow, the heat transfer performance is high, but the pressure loss is much higher. On the other hand, when the arrangement spacing is wide and a / dp = 7.0, the heat transfer surface has a low density, and the heat radiation amount per unit volume is considerably low. Therefore, ▽ in the middle of this data
It can be said that the mark a / dp = 5.0 is the best array pitch structure in terms of overall performance. When a / dp = 5.0 marked with ▽ and a / dp = 6.0 marked with ◇, the arrangement interval b / dp in the air flow direction
Change has a small effect on overall performance, but b / dp is 2
It can be seen that the overall performance is higher, although there are some cases where it is set to about 4.5. This is △ mark a / dp = 3.0
It also applies when a / dp = 4.0 marked with or.

【0016】これら各種配列間隔△,□,▽,◇,○で
の各々の総合性能が高い点付近を結んだ一点鎖線を見る
と、丁度▽印のa/dp=5.0 の付近に変曲点Hがあるこ
とが分かる。この変曲点Hより上側の□,△印のものは
伝熱量が上がるがそれにもまして圧力損失が増大する傾
向にあり、逆に変曲点Hより下側の◇,○印のものは圧
力損失が下がるがそれに比例して伝熱量が低下する傾向
にある。つまり変曲点H付近に丁度ある▽印のa/dp=
5.0 で、且つb/dp=2〜4.5 ピンピッチのもの(図1
に示したピンフィン群11の配列構造のもの)が、送風
動力が小さくかつ伝熱量も大きく、総合性能に最も優れ
た効率の良い放熱フィンと言える。
Looking at the alternate long and short dash line connecting the points where the overall performance is high at these various arrangement intervals Δ, □, ▽, ◇, ○, the inflection point is just around the a / dp = 5.0 marked with ▽. You can see that there is H. The ones marked with □ and △ above the inflection point H tend to increase the amount of heat transfer, but the pressure loss tends to increase, and the ones marked with ◇ and ○ below the inflection point H, on the other hand, show the pressure. Although the loss decreases, the amount of heat transfer tends to decrease in proportion to it. In other words, there is exactly the ▽ mark near the inflection point H a / dp =
5.0 and b / dp = 2 to 4.5 pin pitch (Fig. 1
It can be said that the arrangement structure of the pin fin group 11 shown in 1) is a highly efficient heat radiating fin that has the best overall performance and has a small blowing power and a large amount of heat transfer.

【0017】現実的にLSIなどの放熱器として用いる
場合は、本データ中の▽印のa/dp=5.0 を中心とした
上側の□印のa/dp=4.0 の一部と、下側の◇印のa/
dp=6.0 のものが効率的に許容範囲で、ピンフィン群の
伝熱量を高く維持すると共に、無駄な圧力損失を少なく
できるようになる。この場合にも空気の流れ方向の配列
間隔b/dp=2〜4.5 (針状熱伝導体がピンフィン群の
包絡体積に占める体積割合は20%以下)が適当である。
When actually used as a radiator of an LSI or the like, in this data, a part of a / dp = 4.0 of the upper square centered on the a / dp = 5.0 of the ▽ mark and a part of the lower side ◇ marked a /
The one with dp = 6.0 is an efficient range, and it is possible to keep the amount of heat transfer in the pin fin group high and reduce unnecessary pressure loss. Also in this case, the arrangement interval b / dp = 2 to 4.5 in the air flow direction (the volume ratio of the needle-shaped heat conductor to the envelope volume of the pin fin group is 20% or less) is appropriate.

【0018】なお、前記実施例では針状熱伝導体13の
空気の流れに対し直角方向の配列間隔a/dpは、断面四
角形の角柱の一辺の長さの4.0 〜6.0 倍としたが、断面
五角形などの多角形断面を有する針状熱伝導体を用いる
場合も考え、針状熱伝導体の横断面の外周長の1〜1.5
倍と設定するのが良い。
In the above-mentioned embodiment, the arrangement interval a / dp in the direction perpendicular to the air flow of the needle-shaped heat conductor 13 is 4.0 to 6.0 times the length of one side of the rectangular prism having a square cross section. Considering the case of using a needle-shaped heat conductor having a polygonal cross section such as a pentagon, 1 to 1.5 of the outer peripheral length of the cross section of the needle-shaped heat conductor is considered.
It is good to set it as double.

【0019】[0019]

【発明の効果】本発明の放熱フィンは前述の如く構成し
たから、ピンフィン群の伝熱量を、無駄な圧力損失をく
わせることなく、効率良く高い状態で得ることができ
て、総合性能に優れた放熱器或いは熱交換器を実現可能
とすことができる。
Since the radiating fin of the present invention is constructed as described above, the heat transfer amount of the pin fin group can be efficiently obtained in a high state without causing unnecessary pressure loss, and the overall performance is excellent. It is possible to realize a heat radiator or a heat exchanger.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の放熱フィンの一実施例を示すピンフィ
ン群の一部省略した拡大平面図。
FIG. 1 is an enlarged plan view in which a pin fin group is partially omitted, showing an embodiment of a heat dissipation fin of the present invention.

【図2】同上実施例の放熱フィンのピンフィン群の針状
熱伝導体の最適配列を示すパラメータ実験の測定結果を
グラフで示す説明図。
FIG. 2 is an explanatory diagram showing, in the form of a graph, measurement results of a parameter experiment showing an optimum arrangement of needle-shaped heat conductors of a pin fin group of a radiation fin of the above-mentioned embodiment.

【図3】一般的な放熱フィンのピンフィン群を示す概略
構成図
FIG. 3 is a schematic configuration diagram showing a pin fin group of a general radiation fin.

【図4】従来のピンフィン群の配列状態をしめす一部省
略した拡大平面図。
FIG. 4 is an enlarged plan view showing a state of arrangement of a conventional pin fin group, with some parts omitted.

【符号の説明】[Explanation of symbols]

11…ピンフィン群、13…針状熱伝導体、a…空気流
れに対し直角方向の配列間隔、b…空気流れ方向の配列
間隔。
11 ... Pin fin group, 13 ... Needle-like heat conductor, a ... Arrangement interval in the direction perpendicular to the air flow, b ... Arrangement interval in the air flow direction.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 多角形断面を有する針状熱伝導体を多数
本相互に間隔を存し矩形配列することによりピンフィン
群を構成してなる放熱フィンにおいて、前記ピンフィン
群の針状熱伝導体の少なくとも一方向の配列間隔を、該
針状熱伝導体の横断面の外周長の1〜1.5 倍の範囲内に
設定したことを特徴とする放熱フィン。
1. A radiation fin comprising a pin fin group formed by arranging a plurality of needle-shaped heat conductors having a polygonal cross section in a rectangular shape with an interval between each other. A radiating fin, wherein the arrangement interval in at least one direction is set within a range of 1 to 1.5 times the outer peripheral length of the cross section of the needle-shaped heat conductor.
【請求項2】 ピンフィン群の針状熱伝導体の占める体
積が、該ピンフィン群の包絡体積の20%以下であること
を特徴とする請求項1記載の放熱フィン。
2. The radiating fin according to claim 1, wherein the volume occupied by the needle-shaped heat conductor of the pin fin group is 20% or less of the envelope volume of the pin fin group.
JP10576592A 1992-03-31 1992-03-31 Heat dissipating fin Pending JPH05280882A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10576592A JPH05280882A (en) 1992-03-31 1992-03-31 Heat dissipating fin

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10576592A JPH05280882A (en) 1992-03-31 1992-03-31 Heat dissipating fin

Publications (1)

Publication Number Publication Date
JPH05280882A true JPH05280882A (en) 1993-10-29

Family

ID=14416288

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10576592A Pending JPH05280882A (en) 1992-03-31 1992-03-31 Heat dissipating fin

Country Status (1)

Country Link
JP (1) JPH05280882A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100388050B1 (en) * 1995-11-30 2003-10-11 삼중테크 주식회사 Adsorption-type solution cycle making use of ejector
JP2010221310A (en) * 2009-03-19 2010-10-07 Seiko Epson Corp Turning arm with heat radiation device and horizontal articulated robot
JP2010221340A (en) * 2009-03-24 2010-10-07 Seiko Epson Corp Horizontal articulated robot
CN102519294A (en) * 2012-01-17 2012-06-27 魏辉 Heat exchange unit
JP2013252611A (en) * 2013-09-24 2013-12-19 Seiko Epson Corp Arm and robot

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100388050B1 (en) * 1995-11-30 2003-10-11 삼중테크 주식회사 Adsorption-type solution cycle making use of ejector
JP2010221310A (en) * 2009-03-19 2010-10-07 Seiko Epson Corp Turning arm with heat radiation device and horizontal articulated robot
JP2010221340A (en) * 2009-03-24 2010-10-07 Seiko Epson Corp Horizontal articulated robot
CN102519294A (en) * 2012-01-17 2012-06-27 魏辉 Heat exchange unit
JP2013252611A (en) * 2013-09-24 2013-12-19 Seiko Epson Corp Arm and robot

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